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JP4962837B2 - Infrared sensor manufacturing method - Google Patents
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JP4962837B2 - Infrared sensor manufacturing method - Google Patents

Infrared sensor manufacturing method Download PDF

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JP4962837B2
JP4962837B2 JP2006049492A JP2006049492A JP4962837B2 JP 4962837 B2 JP4962837 B2 JP 4962837B2 JP 2006049492 A JP2006049492 A JP 2006049492A JP 2006049492 A JP2006049492 A JP 2006049492A JP 4962837 B2 JP4962837 B2 JP 4962837B2
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infrared sensor
manufacturing
thin film
forming
laser beam
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JP2007225532A (en
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哲男 土屋
進 水田
俊弥 熊谷
得人 佐々木
晴次 倉科
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NEC Corp
National Institute of Advanced Industrial Science and Technology AIST
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Priority to CNA200710084313XA priority patent/CN101034011A/en
Priority to US11/710,962 priority patent/US7781030B2/en
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/10Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors
    • G01J5/20Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors using resistors, thermistors or semiconductors sensitive to radiation, e.g. photoconductive devices

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  • Spectroscopy & Molecular Physics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
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Description

本発明は、赤外線の入射光を吸収することにより温度を変え、その温度変化により電気抵抗値を変えることによって赤外線の放射強度の信号を読み出すボロメータ方式の非冷却型赤外線センサの製造方法に関する。   The present invention relates to a method of manufacturing a bolometer-type uncooled infrared sensor that changes a temperature by absorbing infrared incident light and reads an infrared radiation intensity signal by changing an electric resistance value according to the temperature change.

ボロメータは基板材料から熱的に隔絶された金属あるいは半導体薄膜の電気抵抗の温度変化を利用するものである。一般に、このボロメータ用材料の電気抵抗の温度係数(以下、TCRと呼ぶ)が大きくなると感度が向上し、赤外線センサの温度分解能(NETD)が小さくなる。   A bolometer utilizes the temperature change of the electrical resistance of a metal or semiconductor thin film that is thermally isolated from the substrate material. Generally, when the temperature coefficient of electric resistance (hereinafter referred to as TCR) of the bolometer material is increased, the sensitivity is improved and the temperature resolution (NETD) of the infrared sensor is decreased.

ニッケル鉄合金等の合金薄膜はTCRが0.5%/K程度と小さいため、高感度の赤外線センサに用いるボロメータ用抵抗体膜としては、酸化バナジウム薄膜、ペロブスカイト型Mn酸化物薄膜、及びYBaCu薄膜等の導電性酸化物薄膜が有利であると考えられている。 Since an alloy thin film such as a nickel iron alloy has a small TCR of about 0.5% / K, as a bolometer resistor film used for a highly sensitive infrared sensor, a vanadium oxide thin film, a perovskite-type Mn oxide thin film, and YBa 2 are used. Conductive oxide thin films such as Cu 3 O x thin films are considered advantageous.

これらの導電性酸化物薄膜を対象とした赤外線センサの製造方法は、例えば特許文献1に記載されている。   A method of manufacturing an infrared sensor targeting these conductive oxide thin films is described in Patent Document 1, for example.

特許文献1による製造方法では、Si基板上に空隙を介して形成されるブリッジ構造体、このブリッジ構造体上に形成されるボロメータ用抵抗膜及びこれを含むブリッジ構造体表面に形成される保護層をそれぞれ、金属有機化合物を溶媒に溶解させて溶液状とし、これを塗布乾燥後に、波長400nm以下のレーザ光を照射することによって炭素−酸素結合を切断して分解し酸化物薄膜とするようにしている。   In the manufacturing method according to Patent Document 1, a bridge structure formed on a Si substrate via a gap, a bolometer resistance film formed on the bridge structure, and a protective layer formed on the surface of the bridge structure including the bridge film In this case, the organic metal compound is dissolved in a solvent to form a solution, and after coating and drying, a laser beam having a wavelength of 400 nm or less is irradiated to break the carbon-oxygen bond to decompose it into an oxide thin film. ing.

この製造方法によれば、所定のシート抵抗、抵抗温度係数を持つボロメータ用抵抗膜を得るために、数時間〜数十時間のサーマルアニーリングが必要であった熱処理方法に比べて数分程度のレーザアニーリングで済むことが確認されている。   According to this manufacturing method, in order to obtain a resistance film for a bolometer having a predetermined sheet resistance and resistance temperature coefficient, a laser of about several minutes is required compared with a heat treatment method that requires thermal annealing for several hours to several tens of hours. It has been confirmed that annealing is sufficient.

特開2002−289931号公報JP 2002-289931 A

上記の製造方法では、ブリッジ構造体やボロメータ用抵抗膜及び保護層を塗布法により形成することにより工程数を少なくできるという効果が得られるものの、塗布法は量産に向いていないという問題点がある。   In the above manufacturing method, although the effect of reducing the number of steps can be obtained by forming the bridge structure, the bolometer resistance film and the protective layer by the coating method, there is a problem that the coating method is not suitable for mass production. .

また、酸化バナジウムによるボロメータ用抵抗膜に関して言えば、TCRにおいて改善されるべき余地がある。   In addition, regarding the bolometer resistance film made of vanadium oxide, there is room for improvement in TCR.

本発明は、上記の導電性酸化物薄膜の中でも特に酸化バナジウム薄膜に着目し、量産に適ししかもTCRを改善することのできる赤外線センサの製造方法を提供しようとするものである。   The present invention focuses on the vanadium oxide thin film among the conductive oxide thin films described above, and an object of the present invention is to provide a method for manufacturing an infrared sensor suitable for mass production and capable of improving TCR.

本発明は、赤外線の入射光を吸収することにより温度を変え、その温度変化により電気抵抗値を変えることによって該赤外線の放射強度の信号を読み出すボロメータ方式の赤外線センサの製造方法であり、絶縁基板上に絶縁材料によるブリッジ構造体を形成する工程と、前記ブリッジ構造体上に、乾式成膜法により酸化バナジウム薄膜を形成する工程と、形成された酸化バナジウム薄膜にレーザ光を照射することによりその材料特性を変化させ、電気抵抗率について1Ω・cm以下とする工程と、材料特性の変化した酸化バナジウム薄膜を所定のパターンに形成する工程と、所定のパターンに形成された酸化バナジウム薄膜及び前記ブリッジ構造体上を覆うように絶縁材料による保護層を形成する工程とを含むことを特徴とする。 The present invention is a method of manufacturing a bolometer-type infrared sensor that changes a temperature by absorbing infrared incident light and reads a signal of the infrared radiation intensity by changing an electric resistance value according to the temperature change. A step of forming a bridge structure with an insulating material thereon, a step of forming a vanadium oxide thin film on the bridge structure by a dry film forming method, and irradiating the formed vanadium oxide thin film with laser light. alter the material properties, a step shall be the following 1 [Omega · cm for electrical resistivity, and forming a vanadium oxide thin films changes in material properties in a predetermined pattern, vanadium oxide thin film and formed in said predetermined pattern Forming a protective layer made of an insulating material so as to cover the bridge structure.

本発明による製造方法においては、前記乾式成膜法として、スパッタリング法、真空蒸着法、CVD法のいずれかを用いる。   In the manufacturing method according to the present invention, any one of a sputtering method, a vacuum deposition method, and a CVD method is used as the dry film forming method.

本発明による製造方法においては、前記ブリッジ構造体及び保護層が、CVD法により形成されたSiN薄膜、SiON薄膜のいずれかであることが好ましい。   In the manufacturing method according to the present invention, the bridge structure and the protective layer are preferably either a SiN thin film or a SiON thin film formed by a CVD method.

本発明による製造方法においては、前記レーザ光として、波長157〜550nmの範囲のレーザ光、好ましくは波長222〜360nmの範囲のレーザ光を用いることが望ましい。   In the manufacturing method according to the present invention, it is desirable to use a laser beam having a wavelength of 157 to 550 nm, preferably a laser beam having a wavelength of 222 to 360 nm, as the laser beam.

本発明による製造方法においては、前記レーザ光の照射エネルギーが、10〜150mJ/cmの範囲、好ましくは30〜60mJ/cmの範囲であることが望ましい。 In the production method according to the present invention, the irradiation energy of the laser beam is in the range of 10~150mJ / cm 2, it is desirable that preferably in the range of 30~60mJ / cm 2.

本発明による製造方法においては、前記レーザ光の照射を、基板温度350℃以下、好ましくは室温で行うことが望ましい。   In the manufacturing method according to the present invention, it is desirable that the laser light irradiation is performed at a substrate temperature of 350 ° C. or lower, preferably at room temperature.

本発明による製造方法においては、前記レーザ光の照射を真空あるいは還元性の混合ガス雰囲気中で行うことが好ましい。   In the manufacturing method according to the present invention, it is preferable that the laser beam irradiation is performed in a vacuum or a reducing mixed gas atmosphere.

本発明によればまた、上記のいずれかの製造方法により製造された赤外線センサが提供される。   According to the present invention, an infrared sensor manufactured by any one of the above manufacturing methods is also provided.

本発明によれば、量産に適ししかもTCRを改善することのできる赤外線センサを提供することができる。   ADVANTAGE OF THE INVENTION According to this invention, the infrared sensor which is suitable for mass production and can improve TCR can be provided.

以下に、本発明による赤外線センサの製造方法について詳細に説明する。   Below, the manufacturing method of the infrared sensor by this invention is demonstrated in detail.

本発明は、赤外線の入射光を吸収することにより温度を変え、その温度変化により電気抵抗値が変化して、入射した赤外線の強度の信号を読み出す方式であるボロメータ方式の非冷却赤外線センサに関する。   The present invention relates to a bolometer-type non-cooled infrared sensor that changes a temperature by absorbing infrared incident light, changes an electrical resistance value due to the temperature change, and reads an incident infrared intensity signal.

そして、絶縁基板上に空隙を介して形成されるブリッジ構造体上に、乾式成膜工程を経てボロメータ用抵抗体膜を形成した後、この抵抗体膜に所定の条件のレーザ光を照射することによって材料特性を変化させて金属酸化膜として形成することに特徴がある。ここで、材料特性の変化というのは、金属酸化膜を構成している金属原子と酸素原子の結合を切り、酸素を分離することで、金属酸化膜中の電子の移動が向上する、つまり電気抵抗率が小さくなることを意味する。   Then, after forming a bolometer resistor film on the bridge structure formed on the insulating substrate through the air gap through a dry film forming process, the resistor film is irradiated with laser light under a predetermined condition. It is characterized in that it is formed as a metal oxide film by changing the material characteristics. Here, the change in material characteristics means that the movement of electrons in the metal oxide film is improved by cutting the bond between the metal atoms and oxygen atoms constituting the metal oxide film and separating the oxygen. It means that the resistivity becomes small.

乾式成膜工程としては、スパッタリング法のほか、真空蒸着法、CVD法を用いることができる。   As the dry film forming step, a vacuum deposition method and a CVD method can be used in addition to the sputtering method.

ボロメータ用抵抗体膜としては、酸化バナジウム薄膜を用いる。酸化バナジウム薄膜は成膜温度が500℃以下と低いので製造プロセス上の問題点が少ない。   A vanadium oxide thin film is used as the bolometer resistor film. Since the vanadium oxide thin film has a film forming temperature as low as 500 ° C. or less, there are few problems in the manufacturing process.

一方、ブリッジ構造体及び保護層は、導電性があるとボロメータ用抵抗体膜における電気抵抗率の変化の検出感度がなくなるので、抵抗が大きくしかも赤外線の吸収率の高い絶縁体であるSiN又はSiONによる無機絶縁薄膜を用いる。   On the other hand, if the bridge structure and the protective layer are conductive, the sensitivity of detecting the change in electrical resistivity in the bolometer resistor film is lost, so SiN or SiON, which is an insulator with high resistance and high infrared absorption rate An inorganic insulating thin film is used.

以上の無機絶縁薄膜の厚さは、目的に応じて0.01〜1μm程度の間で変化させることができる。   The thickness of the above-mentioned inorganic insulating thin film can be changed between about 0.01-1 micrometer according to the objective.

上記のブリッジ構造体上に酸化バナジウム薄膜を形成した絶縁基板を真空中あるいは還元性の混合ガスによる雰囲気制御が可能なチャンバー中にセットし、所定範囲の波長、光強度、繰り返し周波数で所定時間だけレーザ光を照射する。すると、既に述べたように、酸化バナジウム薄膜の材料特性が変化する。   An insulating substrate having a vanadium oxide thin film formed on the above bridge structure is set in a vacuum or a chamber in which the atmosphere can be controlled by a reducing gas mixture, and for a predetermined time at a predetermined range of wavelength, light intensity, and repetition frequency. Irradiate with laser light. Then, as already described, the material properties of the vanadium oxide thin film change.

還元性の混合ガスとしては、H、NH、NO等が挙げられる。 Examples of the reducing gas mixture include H 2 , NH 3 , and N 2 O.

レーザ光には加熱効果が少ない紫外線レーザとして、XeF(351nm)、XeCl(308nm)、KrF(248nm)、ArF(193nm)、F(157nm)等のエキシマレーザやArイオンレーザ(第2高調波:257nm)などによる157〜550nmの波長範囲のレーザ光を用いることができる。中でも、レーザの安定性や最大出射エネルギー密度から、222nm〜360nmの波長範囲のレーザ光が、材料特性の変化を均一にすることができる点で好ましい。 As an ultraviolet laser with a little heating effect for the laser light, an excimer laser such as XeF (351 nm), XeCl (308 nm), KrF (248 nm), ArF (193 nm), F 2 (157 nm), or an Ar ion laser (second harmonic) : 257 nm) or the like, a laser beam having a wavelength range of 157 to 550 nm can be used. Among these, from the viewpoint of the stability of the laser and the maximum emission energy density, a laser beam having a wavelength range of 222 nm to 360 nm is preferable in that the change in material characteristics can be made uniform.

また、レーザ光の照射エネルギー(密度)について言えば、波長を変えることで低エネルギーあるいは高エネルギーでの照射が可能で、10〜150mJ/cmの範囲が有効であるが、30〜60mJ/cmの範囲が好ましい。 As for the irradiation energy (density) of the laser beam, irradiation with low energy or high energy is possible by changing the wavelength, and the range of 10 to 150 mJ / cm 2 is effective, but 30 to 60 mJ / cm 2 is effective. A range of 2 is preferred.

レーザ光の照射周波数は、1〜2000kHz、好ましくは1〜100Hzである。これは、工業用の高出力レーザのパルス周波数は通常、1〜100Hzであるが、近年、出力は低いものの高周波数のレーザが提供されており、繰り返し周波数が高くなればそれだけ高速処理が可能になるという理由による。   The irradiation frequency of the laser light is 1 to 2000 kHz, preferably 1 to 100 Hz. This is because the pulse frequency of industrial high-power lasers is usually 1 to 100 Hz, but in recent years, high-frequency lasers with low output have been provided, and high-speed processing can be performed as the repetition frequency increases. Because it becomes.

レーザ光のパルス幅は、10〜200nsec、好ましくは10〜40nsecである。これも、市販のレーザのパルス幅は、通常10〜40nsecであるのに対し、パルス幅を変えることが可能になってきていることによる。   The pulse width of the laser light is 10 to 200 nsec, preferably 10 to 40 nsec. This is also because the pulse width of a commercially available laser is normally 10 to 40 nsec, but the pulse width can be changed.

レーザ光の照射時間は、1秒〜2時間、好ましくは1秒〜30分である。これは、現状のレーザでは10分〜30分程度であるが、出力の低いレーザの場合には2時間程度の照射が最適になる場合も想定されるからである。   The irradiation time of the laser light is 1 second to 2 hours, preferably 1 second to 30 minutes. This is because the current laser is about 10 to 30 minutes, but in the case of a low-power laser, the irradiation of about 2 hours may be optimal.

なお、レーザの照射エネルギーが小さすぎると材料特性の変化が起こらず、また、大きすぎるとアブレーションが起こって薄膜材料が蒸発してしまう。   If the laser irradiation energy is too small, the material characteristics do not change, and if it is too large, ablation occurs and the thin film material evaporates.

また、上記のレーザ光照射の際には、絶縁性基板を350℃以下の温度に加熱することが好ましいが、室温での照射も可能である。   In the laser beam irradiation, it is preferable to heat the insulating substrate to a temperature of 350 ° C. or lower, but irradiation at room temperature is also possible.

以下に、本発明による赤外線センサの製造方法の実施例について図1を参照して説明するが、本発明はこの実施例に限定されない。   Hereinafter, an embodiment of a method for manufacturing an infrared sensor according to the present invention will be described with reference to FIG. 1, but the present invention is not limited to this embodiment.

(実施例)
図1(a)に示すように、読み出し回路が形成されたSi基板1上に赤外で反射率が高いWSi等の金属をスパッタ法で成膜して赤外線反射膜8とした。この赤外線反射膜8の作製には従来技術をそのまま用いた。次に、この赤外線反射膜8上に感光性ポリイミドを塗布し、リソグラフィーによりパターン加工するか、あるいは多結晶シリコン膜をCVD法により形成してパターン加工し、図示の形状の犠牲層9を形成した。
(Example)
As shown in FIG. 1A, a metal such as WSi, which has high reflectivity in the infrared, is formed on the Si substrate 1 on which the readout circuit is formed by a sputtering method to form an infrared reflection film 8. The prior art is used as it is for the production of the infrared reflecting film 8. Next, photosensitive polyimide is applied on the infrared reflecting film 8 and patterned by lithography, or a polycrystalline silicon film is formed by CVD and patterned to form a sacrificial layer 9 having the shape shown in the figure. .

続いて、図1(b)に示すように、犠牲層9上にプラズマCVD法によりSiONによる無機絶縁膜を形成した。このSiON薄膜がブリッジ構造体2となる。   Subsequently, as shown in FIG. 1B, an inorganic insulating film made of SiON was formed on the sacrificial layer 9 by plasma CVD. This SiON thin film becomes the bridge structure 2.

次に、図1(c)を参照して、ブリッジ構造体2上に熱伝導率の小さい金属、例えばTi等をスパッタ法で成膜し、通常の露光、現像、エッチング工程によって配線5を形成した。次に、ブリッジ構造体2上にスパッタリング法により酸化バナジウム薄膜4を形成した後、この薄膜全面に波長308nmのXeclエキシマレーザ光10を50mJ/cm、10Hz、5分間、真空中室温で照射した。続いて、露光、現像、エッチング工程を経て、赤外線反射膜8に対応したブリッジ構造体2上にボロメータ用抵抗体4’(図1d)となる所定パターンの酸化バナジウム薄膜を残した。この結果、レーザ光の照射されたボロメータ用抵抗体4’はその電気抵抗率及びTCRが変化した。 Next, referring to FIG. 1C, a metal having a low thermal conductivity, such as Ti, is formed on the bridge structure 2 by sputtering, and the wiring 5 is formed by normal exposure, development, and etching processes. did. Next, after forming the vanadium oxide thin film 4 on the bridge structure 2 by a sputtering method, the entire surface of the thin film was irradiated with a Xecl excimer laser beam 10 having a wavelength of 308 nm at 50 mJ / cm 2 , 10 Hz, 5 minutes at room temperature in a vacuum. . Subsequently, a vanadium oxide thin film having a predetermined pattern to be a bolometer resistor 4 ′ (FIG. 1d) was left on the bridge structure 2 corresponding to the infrared reflective film 8 through an exposure, development, and etching process. As a result, the electrical resistivity and TCR of the bolometer resistor 4 ′ irradiated with the laser light changed.

次に、図1(d)に示すように、ボロメータ用抵抗体4’を含むブリッジ構造体2の上に、プラズマCVD法によりSiONによる無機絶縁薄膜を形成した。このSiON薄膜がボロメータ用抵抗体4を外部から遮断する保護層6になる。   Next, as shown in FIG. 1D, an inorganic insulating thin film made of SiON was formed on the bridge structure 2 including the bolometer resistor 4 'by plasma CVD. This SiON thin film becomes a protective layer 6 that shields the bolometer resistor 4 from the outside.

この後、半導体における露光、現像によりパターンを形成し、ガスによる乾式エッチングにより犠牲層9に至るスリット状の溝(図示せず)を形成した。引き続いて、このスリットの溝を通して犠牲層9を除去する処理を行うことにより、空隙3が形成された(図1e)。   Thereafter, a pattern was formed by exposure and development in a semiconductor, and a slit-like groove (not shown) reaching the sacrificial layer 9 was formed by dry etching with gas. Subsequently, the gap 3 was formed by performing a process of removing the sacrificial layer 9 through the groove of the slit (FIG. 1e).

このような形成方法によってボロメータ用抵抗体4’が宙に浮いた構造のダイアフラムを形成した。   A diaphragm having a structure in which the bolometer resistor 4 'is suspended in the air is formed by such a forming method.

このセルが赤外線センサとして作動する原理は以下のとおりである。   The principle that this cell operates as an infrared sensor is as follows.

赤外線がセルに入射すると赤外線吸収率の高いブリッジ構造体2及び保護層6で赤外線が吸収され、一部は同構造体を透過した後、赤外線反射膜8で反射されて再びブリッジ構造体2及び保護層6で吸収される。吸収された赤外線は熱となりダイアフラムを加熱してボロメータ用抵抗体4’の電気抵抗を変化させる。   When infrared rays are incident on the cell, the infrared rays are absorbed by the bridge structure 2 and the protective layer 6 having a high infrared absorptance, and part of the infrared rays are transmitted through the structure and then reflected by the infrared reflecting film 8 so that the bridge structure 2 and Absorbed by the protective layer 6. The absorbed infrared rays become heat and heat the diaphragm to change the electric resistance of the bolometer resistor 4 '.

図2は、ボロメータ用抵抗体4’に照射するレーザ光の照射エネルギーが40mJ/cm、50mJ/cm、60mJ/cmの場合について、赤外線センサ(ボロメータ用抵抗体4’)のTCRの温度依存性を測定した特性図である。50mJ/cmの照射エネルギーの場合、室温(300K)前後においてこれまでの2%/Kを超える3%/K程度の良好なTCRが得られる。 2, the resistive element 4 for the bolometer 'irradiation energy of the laser light provided to the case of 40mJ / cm 2, 50mJ / cm 2, 60mJ / cm 2, an infrared sensor (bolometer resistor 4' of the TCR) It is the characteristic view which measured temperature dependence. In the case of irradiation energy of 50 mJ / cm 2 , a good TCR of about 3% / K, which exceeds 2% / K so far, can be obtained around room temperature (300 K).

図3は、ボロメータ用抵抗体4’に照射するレーザ光の照射エネルギーが40mJ/cm、50mJ/cm、60mJ/cmの場合について、赤外線センサ(ボロメータ用抵抗体4’)の抵抗率と照射時間との関係を測定した特性図である。いずれの照射エネルギーにおいても、照射時間2分を超えると電気抵抗率は1Ω・cm以下となり、ボロメータ用材料に必要とされる電気抵抗率の範囲内に入っていた。 3, 'the case where the irradiation energy of the laser light irradiated on is 40mJ / cm 2, 50mJ / cm 2, 60mJ / cm 2, an infrared sensor (bolometer resistor 4' for the bolometer resistor 4 resistivity) It is the characteristic view which measured the relationship between irradiation time. At any irradiation energy, when the irradiation time exceeded 2 minutes, the electrical resistivity was 1 Ω · cm or less, and was within the range of electrical resistivity required for the bolometer material.

図4は、ボロメータ用抵抗体4’に照射するレーザ光の照射エネルギーが40mJ/cm、50mJ/cm、60mJ/cmの場合について、赤外線センサ(ボロメータ用抵抗体4’)の抵抗率の温度依存性を測定した特性図である。 4, 'the case where the irradiation energy of the laser light irradiated on is 40mJ / cm 2, 50mJ / cm 2, 60mJ / cm 2, an infrared sensor (bolometer resistor 4' for the bolometer resistor 4 resistivity) It is the characteristic view which measured the temperature dependence of.

以上の測定結果から、本発明による製造方法において好ましい照射エネルギーの範囲は、30〜60mJ/cmであると言える。 From the above measurement results, it can be said that a preferable range of irradiation energy in the production method according to the present invention is 30 to 60 mJ / cm 2 .

本実施例による赤外線センサは、特許文献1に開示された赤外線センサに比べ、以下の点において優れている。   The infrared sensor according to this example is superior to the infrared sensor disclosed in Patent Document 1 in the following points.

1.ブリッジ構造体及び保護層の材料として、SiO、TiO、Al等に比べて赤外線の吸収率の良いSiN又はSiONを使用したことにより、TCRを改善することができる。 1. TCR can be improved by using SiN or SiON, which has a better infrared absorption rate than SiO 2 , TiO 2 , Al 2 O 3, etc., as the material for the bridge structure and the protective layer.

2.ボロメータ用抵抗体を形成するための酸化バナジウム薄膜の形成を、塗布法ではなくスパッタリング法で行っており、塗布法は工程数が少なくなるものの凹凸のある基板表面には均一に膜を形成できないため量産に適していない。これに対し、スパッタリング法は基板の凹凸に関係なく均一に膜を形成できるため量産に適しているというメリットがある。   2. The vanadium oxide thin film for forming the bolometer resistor is formed not by the coating method but by the sputtering method, and although the coating method reduces the number of steps, the film cannot be uniformly formed on the uneven substrate surface. Not suitable for mass production. On the other hand, the sputtering method has an advantage of being suitable for mass production because a film can be uniformly formed regardless of the unevenness of the substrate.

3.基板温度を、これまでの400〜500℃以下から350℃以下にして低温化を実現している。   3. The substrate temperature is lowered from the conventional 400 to 500 ° C. or lower to 350 ° C. or lower to realize a low temperature.

なお、本発明が上記実施例に限定されず、本発明の技術思想の範囲内において、適宜変更可能であることは明らかである。   It should be noted that the present invention is not limited to the above-described embodiments, and can be appropriately changed within the scope of the technical idea of the present invention.

図1は、本発明による赤外線センサの製造工程の一実施例を説明するための図である。FIG. 1 is a diagram for explaining one embodiment of a manufacturing process of an infrared sensor according to the present invention. 図2は、図1に示された赤外線センサの製造工程においてボロメータ用抵抗体に照射するレーザ光の照射エネルギーを変えた場合について、ボロメータ用抵抗体のTCRの温度依存性を測定した特性図である。FIG. 2 is a characteristic diagram in which the temperature dependence of the TCR of the bolometer resistor is measured when the irradiation energy of the laser light applied to the bolometer resistor is changed in the manufacturing process of the infrared sensor shown in FIG. is there. 図3は、図1に示された赤外線センサの製造工程においてボロメータ用抵抗体に照射するレーザ光の照射エネルギーを変えた場合について、ボロメータ用抵抗体の抵抗率と照射時間との関係を測定した特性図である。FIG. 3 shows the relationship between the resistivity of the bolometer resistor and the irradiation time when the irradiation energy of the laser light applied to the bolometer resistor is changed in the manufacturing process of the infrared sensor shown in FIG. FIG. 図4は、図1に示された赤外線センサの製造工程においてボロメータ用抵抗体に照射するレーザ光の照射エネルギーを変えた場合について、ボロメータ用抵抗体の抵抗率の温度依存性を測定した特性図である。FIG. 4 is a characteristic diagram in which the temperature dependence of the resistivity of the bolometer resistor is measured when the irradiation energy of the laser light applied to the bolometer resistor is changed in the manufacturing process of the infrared sensor shown in FIG. It is.

符号の説明Explanation of symbols

1 Si基板
2 ブリッジ構造体
3 空隙
4 酸化バナジウム薄膜
4’ ボロメータ用抵抗体
5 配線
6 保護膜
8 赤外線反射膜
9 犠牲層
10 レーザ光
1 Si substrate 2 Bridge structure 3 Void 4 Vanadium oxide thin film 4 'Resistor for bolometer 5 Wiring 6 Protective film 8 Infrared reflective film 9 Sacrificial layer 10 Laser light

Claims (7)

赤外線の入射光を吸収することにより温度を変え、その温度変化により電気抵抗値を変えることによって該赤外線の放射強度の信号を読み出すボロメータ方式の赤外線センサの製造方法において、
絶縁基板上に絶縁材料によるブリッジ構造体を形成する工程と、
前記ブリッジ構造体上に、乾式成膜法により酸化バナジウム薄膜を形成する工程と、
形成された酸化バナジウム薄膜にレーザ光を照射することによりその材料特性を変化させ、電気抵抗率について1Ω・cm以下とする工程と、
材料特性の変化した酸化バナジウム薄膜を所定のパターンに形成する工程と、
所定のパターンに形成された酸化バナジウム薄膜及び前記ブリッジ構造体上を覆うように絶縁材料による保護層を形成する工程と、
を含むことを特徴とする赤外線センサの製造方法。
In the method of manufacturing a bolometer-type infrared sensor that changes the temperature by absorbing infrared incident light, and reads out the signal of the infrared radiation intensity by changing the electrical resistance value due to the temperature change,
Forming a bridge structure made of an insulating material on an insulating substrate;
Forming a vanadium oxide thin film on the bridge structure by a dry film forming method;
The material properties are changed by the formed vanadium oxide thin film is irradiated with a laser beam, a step shall be the following 1 [Omega · cm for electrical resistivity,
Forming a vanadium oxide thin film having changed material characteristics into a predetermined pattern;
Forming a vanadium oxide thin film formed in a predetermined pattern and a protective layer made of an insulating material so as to cover the bridge structure;
The manufacturing method of the infrared sensor characterized by including.
前記乾式成膜法が、スパッタリング法、真空蒸着法、CVD法のいずれかであることを特徴とする請求項1に記載の赤外線センサの製造方法。   The method for manufacturing an infrared sensor according to claim 1, wherein the dry film forming method is any one of a sputtering method, a vacuum evaporation method, and a CVD method. 前記ブリッジ構造体及び保護層がそれぞれ、CVD法により形成されたSiN薄膜、SiON薄膜のいずれかであることを特徴とする請求項1又は2に記載の赤外線センサの製造方法。   The infrared sensor manufacturing method according to claim 1 or 2, wherein the bridge structure and the protective layer are each a SiN thin film or a SiON thin film formed by a CVD method. 前記レーザ光として、波長157〜550nmの範囲のレーザ光を用いることを特徴とする請求項1〜3のいずれかに記載の赤外線センサの製造方法。 The method for manufacturing an infrared sensor according to claim 1, wherein a laser beam having a wavelength of 157 to 550 nm is used as the laser beam . 前記レーザ光の照射エネルギーが、10〜150mJ/cmの範囲であることを特徴とする請求項1〜4のいずれかに記載の赤外線センサの製造方法。 Method for manufacturing an infrared sensor according to claim 1, wherein the irradiation energy of the laser beam, a range of 10~150mJ / cm 2. 前記レーザ光の照射を、基板温度350℃以下で行うことを特徴とする請求項1〜5のいずれかに記載の赤外線センサの製造方法。 Method for manufacturing an infrared sensor according to claim 1, wherein the irradiation of the laser beam, and performing at 350 ° C. hereinafter substrate temperature. 前記レーザ光の照射を真空あるいは還元性の混合ガス雰囲気中で行うことを特徴とする請求項1〜6のいずれかに記載の赤外線センサの製造方法。   The method of manufacturing an infrared sensor according to claim 1, wherein the laser light irradiation is performed in a vacuum or a reducing gas mixture atmosphere.
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